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Anomalous transmission of microwave power at FMR through nickel crystals at 4.2°K
1.Current address: Physics Department, Princeton University, Princeton, N.J. 08540.
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6.Thickness variations were determined from relative X‐ray transmission measurements. The mean thickness was determined by fitting the room temperature FMAR transmission data, fig. 1, to theory using the thickness as an adjustable parameter. This method has been shown to be reliable. See B. Heinrich, J. F. Cochran, J. H. Liaw and R. C. Barker. Magnetism and Magnetic Materials‐(1976). AIP Conference Proceedings No. 34. p. 250.
7.The Dynamics of Conduction Electrons by A. B. Pippard, Gordon and Breach, New York (1965).
8.Curvature of the electron trajectories is expected to be unimportant for the geometry used in the present experiments in which the RF electric field and the external magnetic field were parallel and directed along a crystallographic axis of high symmetry. The “effective” electrons which chiefly determine the response to an electric field are those carriers which move nearly parallel to the magnetic field (See Hirst and Prange).
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